$p_\mathrm{T}$-differential production cross section of prompt $\mathrm{D^0}$ mesons in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Result already published in Eur.Phys.J. C79 (2019) no.5, 388, the world-average branching ratio of $\mathrm{D^0 \to K^-\pi^+}$ has been updated. Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395

$p_\mathrm{T}$-differential production cross section of prompt $\mathrm{D^+}$ mesons in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Branching ratio of $\mathrm{D^+\to K^-\pi^+\pi^+}$: 0.0938

$p_\mathrm{T}$-differential production cross section of prompt $\mathrm{D_{s}^{+}}$ mesons in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Branching ratio of $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$: 0.0224

Ratio of $p_\mathrm{{T}}$-differential production cross sections of non-prompt and prompt $\mathrm{D^0}$ mesons in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$ in the rapidity interval $|y|<0.5$.

Ratio of $p_\mathrm{{T}}$-differential production cross sections of non-prompt and prompt $\mathrm{D^+}$ mesons in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$ in the rapidity interval $|y|<0.5$.

Ratio of $p_\mathrm{{T}}$-differential production cross sections of non-prompt and prompt $\mathrm{D_{s}^{+}}$ mesons in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$ in the rapidity interval $|y|<0.5$.

Ratio between the $p_\mathrm{T}$-differential production cross sections of prompt $\mathrm{D^+}$ and $\mathrm{D^0}$ mesons in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|<0.5$. Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395 Branching ratio of $\mathrm{D^+\to K^-\pi^+\pi^+}$: 0.0938

Ratio between the $p_\mathrm{T}$-differential production cross sections of non-prompt $\mathrm{D^+}$ and $\mathrm{D^0}$ mesons in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|<0.5$. Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395 Branching ratio of $\mathrm{D^+\to K^-\pi^+\pi^+}$: 0.0938

Ratio between the $p_\mathrm{T}$-differential production cross sections of prompt $\mathrm{D_{s}^{+}}$ mesons and the sum of $\mathrm{{D^+}}$ and $\mathrm{{D^0}}$ mesons in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|<0.5$. The systematic uncertainty due to the uncertainty on the branching ratios is $p_\mathrm{{T}}$ dependent.

Ratio between the $p_\mathrm{T}$-differential production cross sections of non-prompt $\mathrm{D_{s}^{+}}$ mesons and the sum of $\mathrm{{D^+}}$ and $\mathrm{{D^0}}$ mesons in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|<0.5$. The systematic uncertainty due to the uncertainty on the branching ratios is $p_\mathrm{{T}}$ dependent.

Charm-quark fragmentation-fraction ratio $f_\mathrm{s}/(f_\mathrm{u}+f_\mathrm{d})$ in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$. Obtained by fitting the prompt $\mathrm{D_{s}^{+}} / (\mathrm{{D^+}}+\mathrm{{D^0}})$ ratio with a constant function for $p_\mathrm{T}(\mathrm{D}) > 1~\mathrm{GeV}/c$.

Beauty-quark fragmentation-fraction ratio $f_\mathrm{s}/(f_\mathrm{u}+f_\mathrm{d})$ in pp collision at $\sqrt{s}=5.02~\mathrm{TeV}$. Obtained by fitting the non-prompt $\mathrm{D_{s}^{+}} / (\mathrm{{D^+}}+\mathrm{{D^0}})$ ratio with a constant function for $p_\mathrm{T}(\mathrm{D}) > 2~\mathrm{GeV}/c$.

$\mathrm{d}\sigma_\mathrm{b\overline{b}}/\mathrm{d} y$ estimated from non-prompt $\mathrm{{D^0}}$, $\mathrm{{D^+}}$ and $\mathrm{D_{s}^{+}}$ mesons (black circles of Figure 12) measured in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|<0.5$. The average $\mathrm{d}\sigma_\mathrm{b\overline{b}}/\mathrm{d} y$ (red circle/diamond of Figure 12/13) of the estimates from the single D-meson species is also reported. Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395 Branching ratio of $\mathrm{D^+\to K^-\pi^+\pi^+}$: 0.0938 Branching ratio of $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$: 0.0224

Production cross sections of prompt and non-prompt $\mathrm{{D^0}}$, $\mathrm{{D^+}}$ and $\mathrm{D_{s}^{+}}$ mesons in pp collision at $\sqrt{{s}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $|y|<0.5$. The prompt $\mathrm{{D^0}}$ and $\mathrm{{D^+}}$ measurements are perfromed down to $p_\mathrm{{T}} = 0~\mathrm{GeV}/c$ and no extrapolation has been done (zero uncertainty assigned in the table). Branching ratio of $\mathrm{D^0 \to K^-\pi^+}$: 0.0395 Branching ratio of $\mathrm{D^+\to K^-\pi^+\pi^+}$: 0.0938 Branching ratio of $\mathrm{D_s^+\to \phi\pi^+\to K^-K^+\pi^+}$: 0.0224

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio as a function of $p_{\rm {T}}$ measured in pp collisions at $\sqrt{s} = 5.02$ TeV in the rapidity interval $|y|<0.5$.

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio as a function of $p_{\rm {T}}$ measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $ -0.96\lt y \lt 0.04$.

The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the transverse momentum interval $2 \lt p_{\rm T} \lt 12$ GeV/c and in the rapidity interval $-0.96 \lt y \lt 0.04$.

$p_{\rm {T}}$-integrated prompt $\Lambda_{\rm {c}}^{+}$ baryon cross section in pp collisions at $\sqrt{s} = 5.02$ TeV in the rapidity interval $|y|<0.5$, and in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $-0.96 \lt y \lt 0.04$. First column: The $p_{\rm {T}}$-integrated cross section in the visible (measured) $p_{\rm {T}}$ region, which in pp collisions is $1 \lt p_{\rm T} \lt 12$ GeV/c and in p-Pb collisions is $1 \lt p_{\rm T} \lt 24$ GeV/c. The second (sys) error is from the luminosity uncertainty. Second column: The $p_{\rm {T}}$-integrated cross section extrapolated to all $p_{\rm {T}}$. The second (sys) error is from the luminosity uncertainty and the third (sys) error is from the extrapolation to the full $p_{\rm {T}}$ range.

$p_{\rm {T}}$-integrated ($p_{\rm {T}} > 0$) $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio in pp collisions at $\sqrt{s} = 5.02$ TeV in the rapidity interval $|y|<0.5$, and in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $-0.96 \lt y \lt 0.04$. The second (sys) error is from the extrapolation to the full $p_{\rm {T}}$ range.